JPS6381613A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPS6381613A
JPS6381613A JP22612186A JP22612186A JPS6381613A JP S6381613 A JPS6381613 A JP S6381613A JP 22612186 A JP22612186 A JP 22612186A JP 22612186 A JP22612186 A JP 22612186A JP S6381613 A JPS6381613 A JP S6381613A
Authority
JP
Japan
Prior art keywords
magnetic
alloy
flux density
layers
contg
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP22612186A
Other languages
Japanese (ja)
Inventor
Takahiro Yamamoto
隆洋 山本
Koichi Terunuma
幸一 照沼
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
TDK Corp
Original Assignee
TDK Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by TDK Corp filed Critical TDK Corp
Priority to JP22612186A priority Critical patent/JPS6381613A/en
Publication of JPS6381613A publication Critical patent/JPS6381613A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To permit easy production by forming a 1st Co-Zr alloy layer having high saturation magnetic flux density and contg. Zr at a low ratio on one of the butt surfaces in a gap part, Then forming a 2nd Co-Zr alloy layer having low saturation magnetic flux density and contg. Zr at the ratio higher than in the 1st layer thereon. CONSTITUTION:The magnetic Co-Zr alloy layers 11 contg. Zr at a low ratio are formed on the surfaces in the gap part of a yoke 10 consisting of Mn-Zn single crystal ferrite and the magnetic Co-Zr alloy layers 2 contg. Zr at the higher ratio are formed thereon. An SiO2 gap material is used for the gap part 13. These magnetic layers are formed by an RF magnetron sputtering method. The magnetic layers 12 of low saturation magnetic flux density to change the effective gap are formed on the Co-Zr alloy contg. Zr at the higher ratio and the magnetic layers 11 of high saturation magnetic flux density are formed of the Co-Zr alloy contg. Zr at the lower ratio, therefore, these layers are easily producible by a sputtering method necessitating mere changing-over of targets. Since the magnetic permeabilities of the two magnetic layers exhibit nearly the same high values, the magnetic head having good characteristics is constituted.

Description

【発明の詳細な説明】 (技術分野) 本発明は磁気ヘッドに関し、さらに詳しくは磁気ヘッド
のギャップ部分の構造に関する。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to a magnetic head, and more particularly to the structure of a gap portion of a magnetic head.

(従来技術) 現在、磁気記録再生装置においては、生産コストの低減
、装置の簡素化などの面から、記録と再生を同一の磁気
ヘッドで行う記録再生兼用の磁気ヘッドが広く用いられ
ている。
(Prior Art) Currently, in magnetic recording and reproducing devices, dual-purpose magnetic heads for recording and reproducing are widely used in order to reduce production costs and simplify the device.

磁気ヘッドのギャップ長は、記録時には記録効率の面か
ら大きい方が良いが、再生時には短波長の信号を十分に
再生できるように小さい方が良い、従って、兼用型の磁
気記録ヘッドのギャップ長は各専用′In気ヘッドの中
間に設定されるため。
The gap length of a magnetic head should be large during recording from the standpoint of recording efficiency, but during playback it should be small so that short wavelength signals can be sufficiently reproduced.Therefore, the gap length of a dual-purpose magnetic recording head is To be set in the middle of each dedicated 'In-air head.

記録及び再生のいずれにおいても専用磁気ヘッドよりも
特性が劣るという欠陥があった。
It had a defect in that its characteristics were inferior to that of a dedicated magnetic head in both recording and reproduction.

この問題を解決するために可変ギャップを有する記録再
生兼用磁気ヘッドが提案されている(特開昭60−68
310号等)、すなわち、磁気ヘッドのギャップ部にヘ
ッド本体部よりも飽和磁束密度の小さい磁性層を挿入し
た構造の磁気ヘッドを用い、記録時に印加される大きい
磁束に対してはこの磁性層を飽和させ、それにより実効
的に大きいギャップ長を有する磁気ヘッドとして動作さ
せ、再生時に磁気ディスク等の記録媒体から加わる磁束
に対してはこの磁性層を飽和させず、それにより小さい
ギャップ長を有する磁気ヘッドとして動作させるもので
ある。この可変ギャップ磁気ヘッドは記録及び再生専用
の2個の磁気ヘッドと同等の特性を有する点ですぐれた
ものである。
To solve this problem, a magnetic head for recording/reproducing with a variable gap has been proposed (Japanese Patent Laid-Open No. 60-68
No. 310, etc.), that is, a magnetic head with a structure in which a magnetic layer with a saturation magnetic flux density lower than that of the head body is inserted in the gap part of the magnetic head, and this magnetic layer is used to withstand the large magnetic flux applied during recording. The magnetic layer is saturated, thereby effectively operating as a magnetic head with a large gap length, and the magnetic flux applied from a recording medium such as a magnetic disk during reproduction does not saturate this magnetic layer, thereby causing a magnetic head with a small gap length. It operates as a head. This variable gap magnetic head is excellent in that it has characteristics equivalent to two magnetic heads dedicated to recording and reproduction.

(従来技術の問題点) 上記の可変ギャップ磁気ヘッドのギャップ部近くの構造
は、第1図に示すように飽和磁束密度が大きい高透率磁
性材料より成る本体1と、ギャップ部において本体lの
対向面の一方に形成された飽和磁束布が小さい高透磁率
磁性層2、または第2図に示すように両面に形成された
飽和磁束密度が小さい高透磁率磁性層2,2(第2図)
より成っている0本体1は通常フェライトを基体とする
パーマロイ(Nl−Fe合金)、フェライトを基体とす
るセンダスト(Fe−3I−A1合金)、フェライト等
で構成され、そして磁性層2.2はガーネット等で構成
されている。
(Problems with the Prior Art) As shown in FIG. 1, the structure near the gap of the variable gap magnetic head described above includes a main body 1 made of a high permeability magnetic material with a large saturation magnetic flux density, and a main body L in the gap. A high permeability magnetic layer 2 with a small saturation magnetic flux density formed on one of the opposing surfaces, or a high permeability magnetic layer 2, 2 with a small saturation magnetic flux density formed on both sides as shown in FIG. )
The main body 1 is usually made of ferrite-based permalloy (Nl-Fe alloy), ferrite-based sendust (Fe-3I-A1 alloy), ferrite, etc., and the magnetic layer 2.2 is made of It is composed of garnet, etc.

このように、本体とギャップ部の磁性層とは別々の材料
で構成されるため磁気ヘッドの製造に非常な手間がかか
る。他の問題点は本体と磁性層の材質が異なるために摩
耗が一様にならないで片減りし、特性の変化や目詰りな
どが起きることである。
In this way, since the main body and the magnetic layer in the gap portion are made of different materials, it takes a lot of effort to manufacture the magnetic head. Another problem is that because the materials of the main body and the magnetic layer are different, the wear is uneven and wears unevenly, resulting in changes in characteristics and clogging.

(発明の目的) 本発明は実効的にギャップ長が可変の記録再生兼用磁気
ヘッドを経済的に製造することを目的とする0本発明の
他の目的は片減りのないこの種の磁気ヘッドを提供する
ことを目的とする。
(Objective of the Invention) It is an object of the present invention to economically manufacture a magnetic head for both recording and reproducing with a variable gap length.Another object of the present invention is to economically manufacture a magnetic head of this type that does not wear out on one side. The purpose is to provide.

(発明のJIり 本発明の磁気ヘッドは、 安価なフェライトを本体とし
て用い、そのギャップ部突き合せ面に高透磁率で高飽和
磁束密度のCo−Zr合金層を形成し、次いでその表面
に高透磁率で低飽和磁束密度のCo−Zr合金層を形成
したことを特徴とする。
(JI of the invention) The magnetic head of the present invention uses an inexpensive ferrite as the main body, forms a Co-Zr alloy layer with high magnetic permeability and high saturation magnetic flux density on the abutting surfaces of the gap portion, and then coats the surface with a Co-Zr alloy layer of high saturation magnetic flux density. It is characterized by forming a Co--Zr alloy layer with magnetic permeability and low saturation magnetic flux density.

(効果の概要) 上記の構成によると、高飽和磁束密度の磁性層と低飽和
磁束密度の磁性層とはCo及びZr含有量が違うだけで
あるから同一の製造手法により青磁性層を容易に製造す
ることができ、経済性が高くなり、磁気ヘッドのコスト
を低下することができる。 また青磁性層の機械的特性
はほとんど異ならないから、磁気ヘッドの片減り摩耗が
無くなる。
(Summary of Effects) According to the above configuration, since the magnetic layer with high saturation magnetic flux density and the magnetic layer with low saturation magnetic flux density differ only in Co and Zr contents, the celadon magnetic layer can be easily manufactured using the same manufacturing method. The magnetic head can be manufactured more economically, and the cost of the magnetic head can be lowered. Furthermore, since the mechanical properties of the celadon magnetic layer are almost the same, uneven wear of the magnetic head is eliminated.

(発明の詳細な説明) 本発明者等の研究によると、Co−Zr合金の組成を変
化させることにより高飽和磁束密度の磁性層と低磁束密
度の磁性層を構成できることが判明した。こうした磁性
層は録音、再生時に高透磁率を持たなければならないが
、この磁性合金はこの要求も満足する。
(Detailed Description of the Invention) According to research conducted by the present inventors, it has been found that by changing the composition of the Co--Zr alloy, a magnetic layer with a high saturation magnetic flux density and a magnetic layer with a low magnetic flux density can be constructed. Such a magnetic layer must have high magnetic permeability during recording and playback, and this magnetic alloy also satisfies this requirement.

従来の磁気ヘッドは通常はフェライトを本体に用い、ギ
ャップ部に高透?a率のパーマロ仁センダストを用いる
が、本発明でも本体には安価なフェライトを用い、ギャ
ップ部の少なくとも一方の面に高透磁率で高飽和磁束密
度のCo−Zr合金磁性層を形成し、その上に同等の高
透磁率と低飽和磁束密度のCo−Zr合金磁性層を形成
する。
Conventional magnetic heads usually use ferrite for the main body, with high transparency in the gap. Permalonite Sendust with a ratio of A is used, but in the present invention, an inexpensive ferrite is used for the main body, and a Co-Zr alloy magnetic layer with high magnetic permeability and high saturation magnetic flux density is formed on at least one surface of the gap part. A Co--Zr alloy magnetic layer having equivalent high magnetic permeability and low saturation magnetic flux density is formed thereon.

これらの磁性層は、フェライトヨークのギャップ部突き
合せ面となる部分を基体として周知のスパッタ法による
成膜技術など任意の方法により製造できる。しかし、本
発明では青磁性層が極めて近似した組成を有するから、
同一の手法で青磁性層を形成するのが得策である0本発
明の実施例ではRFマグネトロンスパッタ法を用いた。
These magnetic layers can be manufactured by any method such as a well-known sputtering film forming technique using the portion of the ferrite yoke that will be the abutting surface of the gap portion as a base. However, in the present invention, since the celadon magnetic layer has a very similar composition,
It is advisable to form the celadon magnetic layer using the same method. In the embodiment of the present invention, an RF magnetron sputtering method was used.

好ましい合金組成は高飽和磁束密度の合金についてはZ
r2.O〜10 at%、低飽和磁束密度の合金につい
てはZrが10.1〜20at%の含有量を有するもの
である。Zr含有量がL0at%より少なかったり20
at%を越えると透?+!!率が低下し好ましくない、
しかし一般的には、青磁性層の間に十分な飽和磁束密度
の差があればよい。
The preferred alloy composition is Z for high saturation flux density alloys.
r2. Zr content is 10.1 to 20 at% for alloys with a low saturation magnetic flux density of O to 10 at%. Zr content is less than L0at% or 20
Is it transparent if it exceeds at%? +! ! rate decreases, which is undesirable.
However, in general, it is sufficient that there is a sufficient difference in saturation magnetic flux density between the celadon magnetic layers.

実施例 第3図は本発明の磁気ヘッドの構成を示し、Mn−Zn
単結晶フェライトのヨーク10のギャップ部の面にZr
含有量の少ないCo−Zr合金磁性層11が形成され、
その上にZr含有量の多いCo−Zr合金磁性層12が
形成されている。ギャップ部13には5102  ギャ
ップ材が用いられている。これらの磁性層はRFマグネ
トロンス。
Embodiment FIG. 3 shows the structure of the magnetic head of the present invention, in which Mn-Zn
Zr is applied to the gap surface of the single crystal ferrite yoke 10.
A Co-Zr alloy magnetic layer 11 with a small content is formed,
A Co--Zr alloy magnetic layer 12 with a high Zr content is formed thereon. 5102 gap material is used for the gap portion 13. These magnetic layers are RF magnetrons.

バッタ法により形成されている。It is formed by the grasshopper method.

COにZrを0.1〜20  at%の量で含有させた
Co−Zr合金を製造し、その磁気特性を測定した。第
4図にこの結果を示す。
A Co-Zr alloy containing CO in an amount of 0.1 to 20 at% of Zr was manufactured, and its magnetic properties were measured. Figure 4 shows the results.

飽和磁束密度はZrの含有率に対して直線的に減少する
。 従って、なるべく低いZr含有率を有するCo−Z
r合金を第3図の磁性fi11として用い、2Qat%
に近いZr含有率を有するCo−Zr合金を磁性層12
に用いることにより、磁性層12を録音時に飽和し、再
生時に高透磁率となる可変ギャップ手段として用いるこ
とができる。
The saturation magnetic flux density decreases linearly with the Zr content. Therefore, Co-Z with as low a Zr content as possible
Using r alloy as magnetic fi11 in Fig. 3, 2Qat%
The magnetic layer 12 is made of a Co-Zr alloy having a Zr content close to
By using the magnetic layer 12 as a variable gap means, the magnetic layer 12 is saturated during recording and has high magnetic permeability during reproduction.

なお、実際の可変ギャップ磁気ヘッドは、例えば次のよ
うに構成できる。
Note that an actual variable gap magnetic head can be configured as follows, for example.

ギャップ材     S+02     0.4 pL
ギャップ深さ            10  IL本
体     M n −Z n単結晶フェライト磁性層
11(高Ms)Co  95at$  28  gZr
  5at! 磁性層12 (低Ms) Co  83atl   I
 JJ−Z r  17aH (作用効果) 以上のように1本発明は実効ギャップを変える低飽和磁
束密度の磁性層重2をZr含有量の多いCo−Zr合金
で構成し、高飽和磁束密度の磁性層11をこれに極めて
近似したZr含有率量の少ないCo−Zr合金によって
構成したから、ターゲットを切換えるだけでスパッタ法
で容易に製造できる。また両磁性層の透磁率はほとんど
同一の高い値を示すから特性の良い磁気ヘッドを構成で
きる。さらに、両磁性層の機械特性は極めて近似してい
るから、片減りを生じない。
Gap material S+02 0.4 pL
Gap depth 10 IL body M n -Z n single crystal ferrite magnetic layer 11 (high Ms) Co 95at$ 28 gZr
5at! Magnetic layer 12 (low Ms) Co 83atl I
JJ-Z r 17aH (Function and Effect) As described above, 1 the present invention consists of a low saturation magnetic flux density magnetic layer 2 that changes the effective gap made of a Co-Zr alloy with a high Zr content, and a high saturation magnetic flux density magnetic layer. Since the layer 11 is made of a Co--Zr alloy with a low Zr content which is very similar to this, it can be easily manufactured by sputtering by simply changing the target. Furthermore, since the magnetic permeabilities of both magnetic layers exhibit almost the same high values, a magnetic head with good characteristics can be constructed. Furthermore, since the mechanical properties of both magnetic layers are extremely similar, no uneven wear occurs.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図及び第2図は従来の変動ギャップ磁気ヘッドのギ
ャップ部近傍の断面図、第3図は本発明の変動ギャップ
磁気ヘッドのギャップ部近傍の断面図、及び第4図は磁
性層の組成と磁気特性の関係を示すグラフである。
1 and 2 are cross-sectional views near the gap of a conventional variable gap magnetic head, FIG. 3 is a cross-sectional view of the variable gap magnetic head of the present invention near the gap, and FIG. 4 is a composition of the magnetic layer. It is a graph showing the relationship between magnetic properties and magnetic properties.

Claims (3)

【特許請求の範囲】[Claims] (1)ギャップ部の突合せ面の少なくとも一方に、高飽
和磁束密度でZr含有量が少ないCo−Zr合金第1層
を形成し、次いで低飽和磁束密度で第1層よりもZr含
有量が多いCo−Zr合金第2層を形成したことを特徴
とする磁気ヘッド。
(1) Form a Co-Zr alloy first layer with a high saturation magnetic flux density and low Zr content on at least one of the abutting surfaces of the gap part, and then form a Co-Zr alloy first layer with a low saturation magnetic flux density and a higher Zr content than the first layer. A magnetic head characterized in that a second layer of Co--Zr alloy is formed.
(2)第1層は2.0〜10.0at%のZrを含有し
ている前記第1項記載の磁気ヘッド。
(2) The magnetic head according to item 1 above, wherein the first layer contains 2.0 to 10.0 at% Zr.
(3)第2層は10.1〜20at%のZrを含有する
ものである前記第1又は2項記載の磁気ヘッド。
(3) The magnetic head according to item 1 or 2 above, wherein the second layer contains 10.1 to 20 at% Zr.
JP22612186A 1986-09-26 1986-09-26 Magnetic head Pending JPS6381613A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22612186A JPS6381613A (en) 1986-09-26 1986-09-26 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22612186A JPS6381613A (en) 1986-09-26 1986-09-26 Magnetic head

Publications (1)

Publication Number Publication Date
JPS6381613A true JPS6381613A (en) 1988-04-12

Family

ID=16840168

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22612186A Pending JPS6381613A (en) 1986-09-26 1986-09-26 Magnetic head

Country Status (1)

Country Link
JP (1) JPS6381613A (en)

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